Machine for measuring unbalance in a rotative body



April 1931- H. B. MCCABE 1,800,553

MACHINE FOR MEASURING UNBALANCE IN A ROTATIVE BODY Filed Aug. 26, 1929 8 Sheets-Sheet l 2 //Vl/NTOfi-' HOB/405B. M CABE,

% fiY/bbfim H. B. M CABE April 14, 1931.

MACHINE FOR MEASURING UNBALANCE IN A ROTATI VE BODY Filed Aug. 26, 1929 8 SheetsSheet 2 /NVENTOR:

HORACE B. MCABE, BY/I'AAM, W)SVM+W A TTORNEYJ April 14, 1931. H. B. MOCABE 1,800,553

MACHINE FOR MEASURING UNBALANCE IN A ROTATIVE BODY Filed Aug. 26, 1929 8 Sheets-Sheet 3 n F I F"" N Z film" II II 1| 1| ||||||||||Hll| II III II ll] ll lllllml HORACE 5. AFC/15E,

A TTORNEYS Ail-n 1 4, 1931.

' H. B. M CABE Filed Aug. 26, 1929 8 Sheets-Sheet 4 FIG 6 'l/VVENT R:

. HORACE a. MCCABE K3 BY AA 4 *W ATTORNEYS April 14, 1931. H.' B. M CABE ,8 ,5

MACHINE FOR MEASURING UNBALANCE IN A ROTATIVE BODY Filed Aug. 26, 1929 8 Sheets-Sheet 7 INVENTORI HORACE B. MCABE,

BYM 040,6 4, am ryz April 14, 1931. B, MCCABE 1,800,553

MACHINE FOR MEASURING UNBALANCE IN A ROTATIVE BODY Filed Aug. 26, 1929 8 Sheets-Sheet 8 I my 18/ FIG. 24 I76 /92 /93 183 a 90 9l 1 me /N VE N TOR 0 HORACE a. M CABE, BY Wfiwvfim A TTOFNEYS patented Apr. 14, 193i ATENT 10F FflCfE l HDBAQEBHMQQABEMQF.MADI Q W CO S N, ASSIGNOR TOrEVAM D S WISCONSIN Applieation filed August 26,:1929. Serial :No..'38,8,;391.

Ehe intention irelates to 1imp 'QVeII16ntS in .maehines for measuring rote iv aln la and apartiquljanly :to :that class :in which .the unbalanced :hocly tot-be tested is rotated in M3 rbearings'alttaohedftola sltpp0rtQ1 fra h is pivoted to oscillate about an flX p rpenflicnlalvto:the axismfqrotation. Inmachines of ithis class :the aeentri-fugal force generated *lgyfthe :rotation actsronzthe pivoted frame -t0 (produce a tu'rningjmoment about ithe ;piv ota,l axis, =and :tl1e::1nagnitu de of ,the corrections to :be.appliedttosthebrotativerboclyrtolefieet a con- -clitiomo-f balancegis iLSCQIIta R y;m6aSuring this turning moment.

can

improved balaningmachinethat will besensitive and zrespondto slight degrees of un balance, andlhyywhich theymagnitllde and position for correction formnbalance maybe wquickly ascertained by a method of direct measurement.

"The invention possesses several ,important tfeaitures which will be brought-1on1; clearly .in'the following speeifioations by the aid of .the accompanying drawings. In the drank vings Lhaveshown-one form. of themachinein xvhiclrthe-rotating;boclytisieonstnaineclto os :cillate insa:horizontalplanemnclerrthe control efsaztorsion springfbut itfis understood that -.I do not limit Vmysel-flto this iorm, since the invention as set EfOftl'l in the claims may ,be

emhodietcljn other forms wherein the body oscillates ,zin :a vertical plane and under the control OfzRD-YOthQI type of spring.

:Referningito thesaicl drawings:

Fig. 1 is=a planview,iFig. 2 airont'elevaationzandzFig. 3 an encltelevation-ofvthelmachine 4L :TlS :a :cross section on the llineaH, {anti iliig. 5 cross: section on. the line 5.5 20f rEig fitis a detache'clfrontwiewl oi the mechranismonrtheend ofthe frame bein-g partially fin section on the line 66 of-'Fig, 3-ancljclrawn to an enlarged scale to nlearly disclose the 1])0fl-i011 of the mecha-nismzshowninrthe sec- ;tional mortion.

lisra SQQtiOIlnOD line 8+8 in Fig. 2,\b,0th. being plan "views 0f-the mechanlsm known as the illhe object ofthe-invention isltoprovicle an elevation ofaltletahetlportion of the damplower-spring pivot, and bofih :beingdrawn to anenlargedzsea eyEig. ,-9 is resection on the ,linei9--.9 in Big. 2 d wn to a enlarged scale, and showing the manner in which the rotary .motion transmitted :from an electric motor to the a griving shaft on the. oscillating frame anem- GI.

.Eig- 10 ,is a ,fronteleva iony nd Fig- ,11 a a plain View o t spe d t-go e t li g ,m' c ami m, -.b0. -h i ws being vrlr w to :the same enlarged-scale.

Eigr 2 is an en .line ;12-'12lof:Eig. ,10. h r

Fig. 13 is a vertical section jf the speed ggoverning evi e 0n :the neu er li e .l --1 of Fig. .11.

rEigl g-is .enIargedre eYatiQnNandIig. loam-enlarged end ne of detail ofthespeed g v rni g mechani mbshowninZFigs- IQ, .11, 1- and :1

Fig- 16 i .aiiront,l vationnimos il ation clamping device. and amp itud indipatorig. 17 is. an. and .v ewoi the clamping d vice and amplitude intlioator, fbeing a sec- .7 .tion omline17-l7 of B g-.16- Rig. 1. isaplanyiewisoif the damping device,'.ib.eing a section n h line "11 -618 in .Fig..

Fig. 19 is v a .vliew lnOking lirom .the reverse so .directiemof Ythed um mem e in m h i shown in Fig. 17,.

.Figs- .20, 21,22, and ar v w on an -:-en1ar,ge.d g ca e 'Qf iasletache l n 6f h mechanism,Eig- 2.0;lb ing an enid V ew as se n rfromltheileftllilE g-2- Eig-21ap1 w, ;-Fig. .ZZanend .view.,. 'h0Wi g h r Side from thatps'hown 'inIEig.;'20 and Fig.2?) an ew in section on .the

in "Fig 2 ig. 24:.i-s. a ,YiQW: Of an auxiliary part used :in nnection with th .m s w ,inlEigs. J20 jto I23 ZinQlusi e.

TFigJQfiiis a plan vieW and Figx26 aifront ing 1Clevice, 11901 1 views ibeing drawn ito an enlargetl seale.

fEig. ",27lis .ai-seetiononfthe line 27-}27 of ,Fig.f25,-, heing ,drawn to the same scale. s

2,8 islasine curve diagram-to'be-re- Th ri e s f'whichthebody to be tested is rotatably' comp r'tively s between {the I; The, only manner in which this resultant force ma ifests 'itselftis massferredtoin' connection with the explanation of the fundamental principles on which: the

V invention is based.

tion ofthemethod employed for determining 1 the phase angle of unbalance.

Figures .1 to 5 inclusive areall drawn to thesame, scale Figures 6 to 13 and. 16 to 24k inclusiveare drawn uniformly to an enlarged f scale of about three to one over that of 'Figures 1 to 5 .1 Eigures 14, 15,25,26 and 27 ,Y

- Inspe'ctionofthe drawings will reveal that essentially-the mach'ine consists of a heavy.

. base towhich is attached a rigid upright sup -po'rting member on which is mounted a'pair' fofv fpivots, disposed in vertical alignment.

are drawn to a still more enlarged scale,

being about two to oneiover that of Figures (Ste 13..

support a" frame membe'r on mounted in suitable bearings. ,With this are "-pivoted frame amanner as to control c the movement" of; the latter land; produce a" system that will oscillate in free. oscillating rangement, the'frame member, and the'rota 1 'i'n a horizontalplane' about a vertical. axis -.th 0u t p votspivots is such that tive body: are capable of? Oscillating motion The. constrnction ofzthe the frame will oscillate freely withoutany appreciable retarding effect dueto friction,

supporting member and the ahorizontal plane angular harmonic 7 tation, an I 'ticnidependingcn' the stiffness of the s i @HdTin' e i r orr p in to that e d'withafnatural period of oscillaa torsion pendulum.

*In this specificati nll will nse the term Qmaterial removed'in' the process" of" 'correct- .zing vthe -.unbalance, in a1 rotative body. In @order -tojdetermine the magnitude for cor necessary I Twill be, constan 7 and the displacement T j willgtherefore be; directly proportional to to measurethelmagnitude and di- 'rection of the resultant .of all centrifugal forcest at action "its; axis 'during rotation.

I "throughdisplacement of In the *cajsefofthe machine to. be; de-

dependsupon the magnitude of t 'l b i d ingWhk the sys em aboutthellpivotal' axis. Under conditions in which the speed of rotation is constant, the resultant .force'fa'nd'theftime the: moment a of inertia "of thejframe and its of sensitivity,

tiff springis connected d 1 eratedacts on theaxis of rotation in" a con-'" s tantly changing radial direction Butthe body 'isbeingrotated is confr mew h h strainedtoswlng'aboutilts PIVOtalELXlS in a load, about the vertical pivotal axisl lt follows that, in order to obtain the maximum displacement,

the moment of inertia of the oscillating system must be made lasxlow as possible; With this point in view the pivoted ,frame member in the machine here described,

is so-designed as to reduce the moment of inertia to an extent with rigidity, power to rotate stead of being mounted on the frame, is attached to the base ofthe" machine.

.In order that a (maximum thepiyoted frame memberbe free to turn on thepivots with a minimum of frictional retarding efiect,"and withoi t'being influenced on the oscillating movement of thefram'e whilethebodyis being'rot'ated." With this reqmrem'ent' in fnind, a novel form of. transmission gearingh'as been developed, which is a feature of the invention to be later: describedqfi i i In an unbalanced 'body'being tested ionthe machine, the resultant centrifugal force genhorizontal plane only, so itis onlythe horizontal component of'fl'the centrifugal I force generated that "acts on the pivoted frame .to

effect aiigular 'di'splacement thereof. 'During a. half revolutioni of the unbalanced body,

I .as great as compatible andthemotor which furnishes the body being tested, in-:

or in other words the maximum d displacement may be obtained, it is further necessary that I so designed' as to produce no appreciable retard ng I or acceleratlng effect this horizontal component-varies from aero,f

which occurs where-the centrifugal force is acting in a verticalfdirection, to 'a maximum value that is' equal,- to the 'centrif igal force, Iand'o'ccurswhen thesame is acting in a horiizontal direction; Now in; measuring unbalance in a machineofthi's type, what we actually deal with is not "this "horizontal component, but-rather the moment of same about the pivotal axis of the oscillating-frame. However it s easier to think of'a force than it is 'to'think 'ofthe moment of-force, so' for the sake ofclearness and brevity I' will herein refer to this moment as aforce, and desig-g na'teit by the letter f. 1 Therefore, Where the force f is-mentioned,it must'be understood to mean the moment of the horizontal component ofjthe centrifugalflforce about the v g i Further; the displacementof the framedue toforce f is angular'displacepivotal axis.

ment; but it'gi's nore 'fconvenient to call it simply displacement so, whendisplacement of the'frame'is mentioned herein, it should be understood that-angular displacement about thepivjotal axis is ineant IE or the same reaife'oogass sons the "angular velocity V of the frame *While oscillating will be ca lle d simply velocity. 1 will designate the displaccment by theich'aractor 19, and the "velocity of oscillation by thelettero.

In cases vvhere the unbalance-of the bod-y beingtested is slight, the extent toxvihich "the force will manifest itself in displacement will be correspondingly slight, and may be "(if 'su'ch extremely small magnitude as to he tliffi'cult to measure. It can be "demonstrated that the" clisplacementdue tothe force intlefperrdentof the speed of rotation depending only ont'he'moment of inertia of the oscillat- 'ing system. it istheretore evident that increasing the speed of -rotation will :not help the "situation, so it is common *practicejin balancing machines 'to {take advantage 'ofthe hiiildingup of displacement that occurs when thefspefed o fro'taftion is 'suchthat one revolution takes "place in the exact time 'ofthc natural period "of the frame with its load. This isknown'a's' resonance speed, and at this speed very smallin-crements of displacement are added indefinitely. Ii rotation is-continuous at this speed the di placement will build up untiltheforce f is neutralized by certain damping forces which become appreciable where the displacement becomes excessive.

In order'totakeadv'antage of this huilding u'p phenomenon't'hatoccurs at resonancespeed it is ievi'dentl'y'ver'y necessary ,to be'ahle to adjust the 'speed with a fine degree of accuracy, an'dftomaintain resonance speed for an appreciable length of time so that-readiingsfor 'displa'cementmay be'taken. To meet tliis requirement'l have devised a novel form offspeedradjusting and governing mechanism which constitutes another novel feature of F tional to, and exactly in phase with the-displacement. .l i'the balancingmachima, where an unbalanced body-is rotated-on a pivoted iram'e, this spring forcehas superposed upon it the'force f, dueto the rotation. Thisi'orce fisalsoa harmonically varying forcefbut itf isaWell established fact that, at resonance speed,itisnot inj phasevvith the displacement, hutlea ds thesame-by almost'exactly a quarter As harmonic motion may be graphically "represented-by a sine curve Ihave shown-in the diagram,Fig. 28, agroup-oi such curves. In-this diagram, distance on the a':-;is 0 rcrepresents*timeflthe"space a others-onrepresenting the period of oscillation; and distance on the axis '0 =y may 'represent any quantity that varies in "a harmonic manner. The curve marked 6 represents the displacement of-the pivotec l'frame, and the-curveimarked f represen'ts'the force f, Wl1lCl1,-t{S 13l1B relative positions of the two curves indicate, leads the displacement bya quarter period, in ac c'ordance with statement in the preceding paragraph. The velocity-oottheirame as it oscillates on its pivots is:a-lso a harmonically varying quantity and it also leads the dis- 'placement bya quarter period, heing' manimum When'the displacement is zero sand zero when the displacement is maximum. The curve o in thediagramirepresents the velocity which, as may be se'en, is in phase with the force Incorporated in the machine constituting this invention is a device for applying :a damping-force, themagnitudeof avhic'hisiexactly proportional .to the velocity 'v. This fforce, avhich I will designatezbyitheiletter 'b, :is in phase with the velocity .and acts irua direction to oppose it. Therefore it :is :evident that it is also in phase with .the force f and acts to oppose same.

In 'the operation 'of the machine, WlJllBtllE unbalanced body is being rotated attresonance speed, the amplitude'of displacement-oi the oscillating frame will build up 'tora point Where the magnitude of the damping force 'Willexactlyequal the magnitude otthe "force f. The dotted'curve b in the figure represents the damping force when :thispoint is reached. The 'force Z),Fbeingi11 phase with and opposing the force f, the effect of the-late ter Will ithenbecompletely neutralized, and the pivoted frame will oscillate under #the control of the spring alone, and "therefore with pure harmonic motion.

Due "to the character it of :the damping device above referred to, the damping force I) is, proportional to :the ve'locity o. The force f, beingwequal tOzlJllGflfLlIlPlIlg force b,.n1ust also beproportional to-the velocity '0. llhis being :true,-theJ-maximum value not f must :be proportional to the maximum value of -41. Now"the maximum value of fas above ex- :plained, v-isequal to the centrifugal fforce .generatedi'in'the rotating body-being tested, so it follows that the centrifugal force is proportional-tothe'maximumvalue oi'athe velocity '0. .Now it is .a =well lrnown :law of mechanics that when a mass is oscillating Withharmoniomotion,themaximun'rvelocity is ,proportional :tothe maximum displacement. Therefore, ifithe centritugaliorce is proportional to themaximum velocity, it is also proportional tothe maximum displacement. Itiollows that; underlthe conditions above given, the amplitude of oscillation (which is the maximum displacement) may be consideredfameasure o'fthe centrifugal "force. 'Hence the amplitude, multiplied by a suitable constantyivill give the'magnitude of a with :a device for automatically applying correction to apply toithe rotative body he ingftested,-to' efie'ct a condition of; balance incorporated in; the construction of themainsame.- l. g An amplitude meter for measuring the amplitude of oscillation of -the pivoted frame 1 is incorporated in'the construction of the ma chine here described From the amplitude meter reading'the magnitude of the correc tion to apply to the body being tested is obtainedin the manner above explained. The V j above, and at right angles to the spring 9,]

radial direction or phase ofthe correction-is ascertained by method involving thepape plication' of a1provisional. zcorrection,' two measurements ,being'required; The method will be fully describedlater in connection the provisional correction, which device is chine. V 1 -7 Having now described the essential features ofth'e'wmachine and the principles on which its operationis ba'sed, I will'proceed to describe'the constructional details of the machine by (the aid of the drawings; g J ,lr'lhe base,"desi"gnatedlby 'the letter B has rigidly ingf memberE. On this supporting'member 'is'pivotally supported the frame, which is designated as a'unit by theletter-Ap s Theframe-c'omprises two mainzmembers mounted Quit the upright supports,

.viz; the horizontal bar landthe'upright bracket member 2.? Adjustably secured tolthe bar 1' are two uprightsupports 3 3. These 5- supports-gare provided with half bearings adapted to receivethe :journalsof a body to betested; -The bodyflto be testecLwhich, for 1 conveniencewill; hereinafter be referred to the rotor, is hereshownas a' familiar type i c ojfgas engine crankshaft, and is'd'esignated r enumber a Th'upright supports, are'clampedto thebar 1 byme'ans of the boltsBt 3,the heads of which are "slidably fitted in the 'longitu-i J I dinal T slot 5, thusproviding a means where'- byi'the supports may be; located tOQ SU.lt-the spacings of the journa'lson diiferentf-typeso f OtOI'SpJi P V The bracket member 2is secured to'the an" derside of bar 1 by means of two' cap screws 6." It is provided -with'two plate-like projecf tions 71'and8,the facesfan'd ends of which are in vertical alignment The upper-projection 7 extends upward adjacent theside face of bar l asindicated i'n Figuresl and 9; These projections form basesfor the attachment of flat "plate springs lconstitutingfthe pivots on whichtheLframe-A asa unit, oscillates. 'f'

I QTheconstruction of the "spring 'pivotsmay be understood by reference to Figures 7 and s,-*in1iwhich ai e sta eifi Steel! P spring, one end ofvvhich-is clampedsecurely between cap 1 0and projection8 by means of screws l 11, the other, I end being similarly-' clamped between cap and a plate like memvertical plane'in a direction transverse tothe frame v A. Thus, the intersections of the two pairs ofsprings form-2a vertical pivotal axis about which; thefframe A; can oscillate; f i

, V Power'ifor turning the rotor is provided by berm? The Plate c do the-1m;

portion of the supporting member 'E by means of cap screws'14 as indicated. The end faces c 13 of plate 13 and 8' of projection 8 are substantially in the same verticalplane, and the corners of each arerabbetedas shown, so that a-short portion l6ofv spring 9 is free toflex; This constitutes the lower spring pivot on which the frame A oscillates,

Thisis shown clearly in Fig. 7, which figure, being a section on line T-{Yin Fig.2, is alftop view of the complete pivot mechanismas' a unit; Thespringl7 is clamped to the endw face of projection 8 by'meansi offca'p 18 and vscrew 19, and'to'the end face of plate 13. by

means oficap' '20fa1idscrew-21.

An -auxiliaryi flat spring 17 1s disposed 'sprine nd being secured to 'thesupportjE inthe same 9 manner, as may beseen by reference to Fig; 1. The principal spring 9' is clamped to'th'e projection 7 by means of cap "10, and to plate 13vby means of cap 12, these two caps being duplicates of caps 10 and 1'2, and are Secured by means of screws to the membersYand 13' in the same ma'nne'r that caps 10 and 12 are secured to themembers'S and-13; nsane-1 iliar y spring '17 (see Fig.1.9) is a duplicate p in '17. his placed below, spr ngs and liesin .adirection at right anglesto th of 9 asshown; 7 It is clamped to projection 7 bylmeans of clamp 18', and toplate Inember 13 by m'eanszof clamp- 20",; (shown in springs 9' and 17,"which comprise the j upper dottedilinesin Fig. 9,),theseitwo clampsbe- 111g duplicatesof,clamps '18 and 120, and are vpivot are the same; as that of springs 9-Tand 1 '17 which 1 comprise the lower'pivot. The

parts are so positioned that springsQand 9 lie the same "vertical plane in af direction 'longltudlnal with ,respect to the name A,

and the springs c 17 and '17. lie in i the same an electricmotor2l, which is -mounted on a bran h; E. h .7 s pp membe Leeds ton c nnec ing th m t o s urce of? urrent sunply. are, indicatednt 1 5., The motion. is;transmijt ted; through. a; coupling to the-.driveshnftofif an adjustable speed govellllihg device which is designated on the drawings. as. a 11nit;by, the; letter G. From this the motion is, transmitted from spur gearflfi, which is part of. the governing device, toia. like. spr r. ge r. 2 on a: s af wh ch is journalled at o e. nd in. hearing 26in thebracketfn ember 2, and t tthe other in bearing 27, located in. a gem: bracket 28 whichrissecnred to tllfiend ofbar l by means Qt o wsit.

From shstt, 2.5 h mo ion. is nsmitt d ttmoiigh r in. :1. gears mounted on. ge r bracket. 28; to, a, drive" shaft 30. which is. connested. tothe. rotor y mean it uita adnnter which will be later. described.

I wil o pnoeejedt descri e hicle ilthe neohanisnit r transmitting hemo i m from the. adj lstable gore n g, device G t e; to.- ton, leaving the description; oi thisxdevice G and an explanation, of its. operat on. to be taken. up. late Itwill be suflici'ent for the present. to. state that it functions. to, impart a. unif rm spe d f rotation to. the ge r 2 nd provides. a. me s of adi s i g he speed by. thema iphlstion. t and hee LT Referring to. Fig, 9, it may be seen; that he gears 2.3. and 214,. bo e ref rred to, are n: mesh on e li e. ot the pivotal is]? 1? The ar o posi ioned that their p tch ci cles 23. and 2fl-"sre each bs antia ly tangent I to, this, The teeth; on these two, gears iresoiqrmed: as'to r-oyide considerable back lash, and also a, substantial clearance space between the: topsand bottoms of the teeth. In the design of the gears, advantageistaken of the faetthet he. oad on them svery light and hey are a cordingly made with narrow laces. It may e. se n that th constru ion above, described allows. a. imited angular dive gen oi the; p an of gea 24 ith th t of gear 23. Wi hout, producing ny c amp ng condition... Asthe shgent point or the pitch circles. lies. in. th pivot ine. l?P-,. t is q it plain, that motion may be transmitted from near 2.3 to gear 24 wi h t imparting t l sligh est mpulseto modity the osc llation of. fr med on. the pr ng piv ts. and, except tor the efiectoi a ry slight friction etw n the teeth, inmesh (found in practi e. to be negligible), the frame will oscillate with perfect freedom.

On the outer end oi shaft 25 is. mounted a spur gear 32 (see Fig; 6-) and i lso a rotary disc: which be thrown out. of balance a known amount atwill. This device is. designatedas a unit by the letter D, and the mechanism and pnrpose oi same will be later exp ained.

. egbore in the tip-per e d' tg er ck 28;, concentric with the axis of the rotor 4, is tightly fitted stud- 33- (See F g, T i

stud supp s l hear ng 3 of. e. radial type, the outer' race of which fits a concen trio bore in a spur gear 35. The ball} bearing is held p ace i s id; or y of cap member 36, which is secured to the side oi the gear by means of screws as indicated in lligfii The said cap member 36 is bored to form a ring-like wall, may be seen in E-i'g. 6. Threaded in this wall; are two pointed pivot screws 37 radially-disposed and in djia; metrically opposite positions. This cap 36 in.- o ne t on w hth g r 5' ndso ews 7 constitutesthe outer member of a i niyersal joi o he gimbal; yn

T e c nic l poin s of crews ng ge diametrically pp ite countersunk depressions in, :17 ring 38, which constitutes the in termediate member ofjthe nniyersal' joint.

The inner member of the nniyeisal joint s gnated by h ni m e r This e ber is concentrically bored toreceive the rotor driving shaft which serves totransmiit he. 'Otary mo o ge r to the oto The en rged end. t'memb 9 ta ns two set screws 40 oppositely disposed: for the P p se otihaltnoe, T es scr ws s r e. to grip theshaft 30 in any desiredendwise, position. The other end'ofmembei' 39 which liesvwithin the ring member 38, contains two un ers nk depr ss ns, o e f hi h s shown at 41, (Fig. il, the Other being in a di t lletrically opposite location. These de- P ss ons li on s disme rsl xi a is at right angles with the axis of pivot screws 37, and form seats, for, two conically pointed pivot screws, (not shown), similarto screws 37 that are threaded diametrically oppor site holes in the intermediate member 38;

Referring to Figs. 1;; and 2,, 42 designates a apter or co pl ng o the familiar split collar type, which encircles the end of't'he rotolf 1 11 is held gripping contact therewith by means of clamping screws 43, the som b ng oppo itely di po d. to sheet s a ance.

.One he end. of t e coup ng member :2 and integral therewith is a ring-like wall 36', Which constitutesthe outer member of a universal joint, the construction of which is same, asthat oi the above described universal j0int,ex cept that the inner member 39 (corresponding to ember .9), instead; of being adjustable on shaft 30" is; rigidly secured ther to by any suitable means.

he arra g ment f he two niver a joints, one on the driving gear and the other on the rotor, as; indicated, insures smooth runningand absence of any cramping; etlfect due to lack of precise alignment of parts. The shaft 30, being adjustable endwnys in the member 39., enablesthe rotor tobe mounted in any desired position endwise on the frame A.

Referring to. Figs. 3, and 6, the rotary mo.-

ti n of he gea 2 s an mi ted o. ge'e .*The lowerend of torsion rod 47; is adjust? ably clampedjin' a .yerticalflholain' blo'c'lrfiti means 'o'f'a set crewte This block gi'sr secured to the bracket member Qbynieans fo'f i l team; 'theh'ead" of which slidably fi s-a slot -'Y'Oscillatidiiofth frame is controlledby through'the; intermediate hr idle'r' gear' which ismounted on av-studf46 Gears 32' and 35,1haye equal numbers of teeth so the I i 'rotor Will'be turned in unison with thelshaft and also with g'earsl23 and 24'. V v I the fac'efof; a'hub portion .3 5 e.cof the gear isa mark which cooperateswith an index markonthe clip 202 to -indicate av zero. angular position'foi' the rotary ("disc D above referred to. 7

H This is f more clearly seen; in Flgures 1 and 6.

atorsion'rod 47, the upper end of which; is

secured by means ofset screw 48 in a concentrio hole in the enlarged lower end or head 49 of ashort vertical'shaft which is journaled in a hracketfmember 50., This member is se-' cured ,to'the upright support E bymeans' of i thetwo. screws 51fas shown. ,Mounted 'on the said-sho'rtvertic'al shaft at its, upper endis V saidkworm and worm wheel, to head 49,; in

the torsionirod; 47 is clamped, thus t end a tensioned inane direction or the otheratwilh means by whichjthe rodfmay be 1.58 in saidibracketmemben By means of this J 'bolt-iand the set screw '56 the block may be j l securedfin different positions along the slot 58, and the sion constant. I

i I 5:.F r t PU P .se f i d y ni e a d preventin g'oscillation of the frame while v rotors arebeing mounted o'nori removednf rom c "themachine fortesting', a-pillar, designated as a; unit ,bytheletterjF; is, mounted'lon the i 1- basefB" near the'end or frame A: The y member 59' of this pillar containsat'itsfupper aidat 5e, in which is slidably'fitted 1 1 g-- er bolt 60; Means are provided for raising and lowering this bolt a 1imiteddi'stance5 said means comprising a shaft 61, journaled {in a f horizontal bore inthebody member 59, the axis of which-intersects the axi's of bolt 60L 'On 'fthe inner, end ofjsh'aft '61, and-integral f itherewithis an ecc'entricstud 62.; This stud "engages' a transverseislot 63 in the bolt 60; The shaft-Gl is prevented from endwise move- 'Inent'by a transverse pin 64 secured fin the V V hody5 9 which projectsinto' an annulargroove in shaft 61 as indicated plainly in Fig. On

r the outer endiof shaft 61Iis attached anop'er ating handle 65 by which the same 'may bef; turned to actuate the eccentricstud 62 toraise; or lower thejb olt '60," The upper end of bolt 7 rodfclampedinfsaine' to vary the ing shaft 72. working lengthpf the rod and hence its'torv e i of the frame;

' i,so'o,55s

J60iis tapered as shown, and-in its lowermost position rests in closecproximity to the bottom vface 'of'the'bar 1.. The'bolt' is" positioned in axial alignment witha hale 66in the bottom wall of bar 1, the sides of which are tapered to correspond with the said tapered endof the bolt-60. Two upwardly extending studs 67;

rigidlyisecured in .theupper face of the body 7 member 59, and positioned onopp'ositeisides of the bar 1', act as stops for same to prevent the amplitude of oscillation of frame A increasingbeyond predeterminedlimits. In

Fig.6 the bolt 60 is shown in its lowered position, withthebar 1 freeto oscillate. is plain that'when the boltis raised by turning the handle 65, the tapered endwill-enter the h0le 6 6 and lock the barl from oscillation; l I

I will now describe the speedadjusting and governing device G, with reference to 'the detail viewsjo fsame, Figs. 10, 11,12, and 13.

The frame; member comprises a body portion with two upwardly extending branches 68 and 69, and two bracket" like portions 70 and shaft 72' "Rotation is" transmitted tof'this 71. Journaled in the branch 69 isja driving p 390 V shaft from the motor '21 through a coupling,

:(one member of which isfdesignated by the number 73 a shaft 74,'and a-pai btsp irai gears 5 and 76$ The; coupling consists'of a disc73'mou'nted on the'endof themotor shaft,

anda similar disc 7 s' ounteapn the endof shaft-'74, ITheldisc T?) contains a 'radial slot thatengagesa stud 203, asmay be'clearlyl seen in Figuresl and9'. The shaft74 is'j ournaled in the bracket. portion 71f: of the frame and [carries the spiral gear 7 5LfThis gear operatively engages the spiralgear'76 whichis rigidly mountedon the'oute'r end of the driv- 7 2 isjournaled in" the branch 69 V I On the inner en'd of this shaft and integral therewith is a drum portion)?! which; is concentrically bored to fit the. outer race "of a radial" ballIbeari'rigj'ZS. Th e'bore The shaft of the inner;race ofthis' ball bearing I constitutesa bearing for the inner end of a driven shaft 79 the outerend of which is journaled 'in'lthe branch 68: of the frame; Thus,*the

driven shaft 79 'isin axial alignment withthe driving shaft '12, and is free (to turn independjently of the latter; Onthe'shaftm'and adjacent the branch "69 of theframe is mounted the spur 'gear'23'to which reference hasv previously-beeii madetf I On'the inner end i thetdriy en naw a adj acent to the drum 77 is mounted a disc'80,

being, securedv thereto by; means of a taper pin in a hubportion; 81 Located adjacent the face-'80? praise 8O is a brake shoe member 82, the body: portion. of iwhi'ch is substantially rectangular in contour; and is proyidedwith a surface 82'; concave'in form to fit the face of drum-77 and'enga'gefsaine with frictional contact; 7 "Secured to the disc .80 and projecting from the face 80f1ther'eof, is asquare stud Iill igeoowas' face 82- onsaid member to moveoutwardly from contact Witl'rthe face of drum 77. The position ot'st'ud 8-3 is such that the movement ot surface 82- will be substantially in a radial direction".

A coil spring" 87- is connectedbetween a stud 88 that isse'cured in disc 80; and a: stud 89 that is secured in: the brake shoe member 82-; the" same extending therefrom: in a direction substantially opposite-that of the extensi'on 8 l. Considering the assemblage of st'ud 89 member" 82', and extension. 84:- as a lever fulerumed at thestud: 88, it is plain that the coil spring 8? aot'stopress the contacting surl ace 82 into frictional: engagement with the face ofdrum: 7:?

g It may be observed that the device so far described answers: as a: means for transmitting the rotary motion of the driving: shaft 72jto the drivenshraft'fu, through the medium of the frictional engagement of drumii'i with brake shoe- 82r and the connections of SAQTJJG' disc 80'. It may also be? observed that the device? will. function as a speed. gnvernor, for, when: the disc- 80 rotates under the driving force of the trictiFon between the surfers 82. and that of drum 7?, the member 82', being oi? substantial mass-,iwil'lidevelop ai centrifugal force tending to separate the friction surta'ces'. Assuming th-atthc: tension. 01; the? coil spring; 87 is just suitiicient to counteract the centri tli ailforce when the speedoii the disc is: a point somewhat below that of driving shaft T2, itis plain that any; sli'g t increase ot the discspeed above th'atpointi ll easetlt'e press-cu e between the friction: surfaces and allow a slip to take place which will continue until the disc speed reduces to tlieipoint-whcre pressure will: again establish-ed. This action wilt be repeated at very short intervals and the result will be that. a practically una fornr speed, winch: depends on the tension of the coil spring, will be imparted toth-e: driven 11 x xi:

Figs; M and: 1 5: comprises to plate 91,a stud 92iand'twoitrunnions 93". Thetrunnions are made av tight fitiin suitableholes in:tl1o-ends of plate 91 and in. the operation of assembling ane forced into place. The stud. 92. is rigidly secured in; plate 91' and extends at right angles theretoias indicated.

The plate 911; biesparallelitoitlie disc 80, and its inn'en end is provided with" a counterbored opening somewhat larger" in diameter than the. shafitiQi and concentric with. same. This opening; forms the seat fora: coil spring 94: as seen. clearly in Fig; 13; For the purpose of obtaining smoothv rimming, two counter weights 95. ans securediby means 0t screws to the disc- 89 mean the: periphery and. on the face: 89. thereof. They are so disposed in relationitoi the: other. members 1 attached to 1 the disc as to: effect an approximate running balance:

A. circular opening 96 in; plate 80- provides a passage with: substantial clearance! fonthe stud. 921:0 engage the stud 89-asimay be'more clearly seen: Figs; 1'15 and 1:22 litlr this arrangement the pressure of coilspring' 94 em the plate 91 causestlie stud 92 to press outwardly onstud891andi oppose the tension coil: spring 8 '5'011: same, thereby reducing the effective tension on brake shoe! member 82. It is plain that by varying the pressure of coil; spring 94: on plate 9.1 the pressure between the friction surfaces may: be varied and? thespeed of! shafit' 7 9 thereby adjusted. Themechanisnr for varying this spring pressurewilt now bedescribed.v

The end on spring Si l-remote from plate 91 encircles: the shouldered end of a sleeve 97 which slrl'dably' fits shaft '39. This sleeve: is provided with a keyway 98 extending its full length, which; cooperates: with a feather 99 secured in. shaft. 79 to allow tree endwise movement but prevent rotation on same. Mounted on: sleeve 9? is a ball thrust bearing 1000f well known. construction; This thrust bearing is pressed against a shoulder 101 on sleevoSfl the two: arms 162' of a forked memher 103-, which is rigidly secured on a longitudinally disposed bar 194 by means of a taper pin. The bar 104 slides at one end in a bearing provided in a lug'105i that is made integral: with the frame, and at the other end in a suitable bore in the branch 68 of the Ta-met Engaging rack teeth 106, out in bar 105,. is a pinion 107 (Fig. 13) which is fast on the inner end of a transverse shaft 108. The pinion end of this shaft turns in bearing 109 in the frame member and the other end turns bearing 70 in the bracket portion 70 of the frame; 0n the outer end of the shaft 108 is mounted the hand wheel 31 previously referred to. A manually operable means is thus provided, through pinion 107 and rack teeth 106,- to slide the bar 104 endwise in its bearings. The movement of the bar imparted by the hand wheelbeltransmitted means of the forked member:103 'and the ball thrust bearing 100, to'the sleeve ;97 ,thus increasing or decreasing the pressure of coil 7 a e a scale m. Figs. 25, 26,and.27.- The essentialv members of the pivot mechanism in 111118111111] spring 91 on'the bell cranklever It is now plain, in viewof the foregoing explanation ofthe speed governing mechanism mountedv v 7 n the 'disc80, that thespeed of. the shaft .79 anclgea'r 23may be varied at'will by the 'manipulation'of the hand wheel 31. V.

s attached.

tothe upright supporting memberlE,-and is so. located thereon that the gear123 meshes properly withggear 24,1'a's, shown in Fig; 9. 7 Referring tosFig. 1, the frame of the govern 'ing device is secured tot-he member E by means of screw '2 O4 'whic'h passesthrougha the same connectingmedium. Inthedrawingsthe frame 'dampingdevice is designated by the l'etter'K i and the amplitude indicator asv a'whole, by

suitable hole in same andenters the threaded hole 205' in branch '68 (seen in'Fig. 9), "The other screw 2 06] (Fig.1)passes through hole, 207 9)xin the branchGS andenters a suitablegthreaded hole in member "E; 7

5 ,1 'will'now' describe the constructionaof the oscillation. dampingdevice and the amplitude indicating' 'instrument; two units which have been referred to inthe preceding gen-. 1 eraldescription 0fthe machine. Although 'theseiare separate units, for constructional reasonsit ispreferable tc-mount both on the same'supporuandto transmit the oscillating movement of the frame A to them-through member of the f'the'letter; H. Referring particularly to'Figs.

: damping device comprises a'boss' portion 110,

16, 17, 18 and 1 19, the base member of the an upwardlyextending portion-1111 and a laterally extending portion 112.. The boss F110 is bored'to iit'around bar- 113, and ispro- Lvided with a slot .anda clamping-screw 1,1 1

' Y i by whichitmaybe securelygripped in po- Ysition 'o n' thejbar' 113. This'barfi's secured in horizontal-bore in theLsupportingmem- 'LberE by. means-,ofthe two setscrews 115 H screws 121 threaded in'the pole pieces 117 as as ppo-rteforthebase member 1110 and -,anis1n as shown V i ThemagnetM is of'the'well known horseshoe form, having a yokeg116, pole pieces 117 e comprises a-drum-l36=which-isprovided as may'bese'eniin 1, and it thus serves as 1 I the mechanismattached thereto.

1 "Thedampingdevice. consls byVboth ofiwhich are attachedtothe frame K, the latter by means of a .springpivotmechand cores'1 118, the latter-being encircled by coils 119 whichare provided with terminals 11.9C;.-3f0r iconne'ctio'n' in an electric circuit.

v ts'iof electro magnet designated asa-whole by the letter -M, and ajpivoted vane'de'signated' as awhole may. be seen in Figs; '16 and18, the-pole pieces being sopositioned that-an air gap 122 is formedbetween them;

The vane unitV is shown on anenlarged are the-twobars 123 and124. -"Thesebars are rectangular. in form and are fiexiblyflconw.

apart to insure lateral rigidity of the vane.

A third 2 pivot spring 127 5 is, vertically dis- 'posed between the main :pivot'springs' fof the purpose. of 1na-intaining,-proper{align- V ment. --,-The m anner of attaching the pivot springs to bars 123fa-nd 124 :willbe clear by reference to Fig. 27, which beingfa section on linej27 27. in V Fig. 25.dis closes themain pivot asp-ring 125.} The ends of this; spring are rigidly clamped ag ainstfthe. horizontal i faces of therbarsiby means of screws 128 and clamping plates 129, 'these. .memb ersl being identical for-both bars. Thebarshave'their vertical faces in substantial alignment, and

in; order'to provide .free portions-bf the springs for flexing, the corners fof'the bars are provided with: rabbets as JShOW1'l-" The manner of attaching the pther main pivot: spring 126 is, as may be seen, the same as that just described for "spring 125, and as may be seen in Fig. 26, the description, also answers for attaching the Vertical pivot spring"127, the screws and clamping plate.

members being identical for all three springs. An angular bracket member 130 is'secured tothe vertica-l face 131:of'bar .-12'4 by means of two-screws as indicated; *To thefrontside ofthisbra'cket'is secured by means of vane- V oscillates. To the rear side of, the

magnetic metal of high electricallcond-uctiv- "ity, preferably aluminium The bar 128,

which acts as a supportfor the vanelmecha- .jnism as well as for thepivot springs, is secured to the frame K bymeanslof screws 135 'rivets'132 "segment member 2133, so posi tioned that its convex face 'isj concentric with the axis through the intersection of themain and vertical pivit springs,;about which the and is'located'thereonin suchaposition that the bodyportion 1341 of vane 134 will oscillate with clearance within the air gap .122.

The mechanismof the amplitude indicator back plate member 138,".and the front bearing is mounted ona' plate-139 which is supported by two'pillars 140 that-are secured I .in theiback p1a-te1385 'On the front end of drum ismounteda hand or pointer 172' which is counterbalanced by a weight 17 3 attached to a depending portion by means of a rivet as indicated. The pointer 17 2 sweeps a dial 174 which is mounted on four ports plate 138'.

The mechanism as a whole is supported on a vertical post 141 which is secured in a socket bored in an upwardly, extending boss 144 a split bore encircling thepost 1 1-1 and is clamped; thereto by means of a clamping screw 146'. The back platemember 138 of the mechanism is attached to the. bracket 1nember1 l-5 by two screws, one of which is seen at 1 17 in Fig. 3.

A flexible band 148 preferably made of thin spring steel iseinploye'd to effect an operative connection bet-w-een t-he vane V of the damping device unit and the drum 136 of the indicator unit. This band is attached at its upper end'to'the drum 136 on the reverse side of same" as viewed in Fig. 1'? by means of a suitable screw 142. It is wrapped a partial turn about the drum in a counterclock rise direction, and is attached at its lower end to the segment 133" by means of screw 149. (SeeFig. 26'.) Two similar bands 150 dis posed on opposite sides of band 148 are also attached at their ends to thesa'me side of the drum 136 by means of screws that are identical withscrew 142. These bands are wrapped a partial turn about the drumin a clockwise direction and extend upwardly therefrom. The-manner in whichthe-three bands are wrapped about the drum 136 and are securedto same by means of screws 142 is better shown in Fig. 19 which is a View of the drum by itselfand viewed from the reverse side thereof: 1 i

The upper ends of'thetwo bands 150are connected to a spreader bar 152, the ends of same being slitted to receive the bands, which ai'eheld therein by means of small pins as indicated: In a hole 'inba'r 152, midway between the bands 150,-is hooked the lowcrend of-a'coil spring 153,the upper end of same bcillQlIOOlZGCl on a post 154: that is secured in the back plate member 138'. This 0011 spring 153-servesto keep the bands taut, and exerts a torque on -drum 136 that tends to rotate it in' a clockwisedirection; The middle band 14-8, by 1ts connection to the vane V opposes the tension of spring 153 and exerts a torque 'onthe drum-tending to rotate" it in a countercloekwise direction. Thus itis plain that the coil spring 153 serves to keep the bands taut, andith'atan oscillating mot-ion imparted to the-vane V will, through the medium of the 143 on the frame K by means of a set screw Abracket member 145is providedwith bands impart a rotary motion to the drum 136 and cause the pointer 172 to sweep the dial 174.

I will now describe the mechanism connecting the pivoted frame A with the vane V, by which the oscillating motion is transmitted and changed from a horizontal to a vertical direction. The mechanism comprises a sector which is pivotally supported by means of a spring pivot mechanism comprising three pivot springs secured to two bars by means-of screws and clamping plates, all of which are identical with corresponding members in the above described spring pivot mechanism forming part of the vane unit. The bar 123 corresponds to bar 123 and bar 124; to bar 12 1 in the previously described mechanism, the bar 123 being attached to the laterally extending portion 112 of the base member by means of two screws 156.

The sector member 155 is secured by means of screws 15? to the under face of bar 124'. The faces 158 and 159 of the sector member are concentric with the axis through the spring pivot and have equal radii. To the lower end of face 158 is attached by means of screw 158 a thin flexible steel band 160, which extends upward and, through the means of a coupling 161 is joined to a band 162, the upper end of which is attached by means of a screw 163 (see Figs. 25 and 26) to the upper end of segment 133 on the vane unit- V. A similar band 164: attached to face 159 by means of screw 165 extends in a horizontal direct-ion and connects to the bar 1 of frame A. The connecting means consists of a bracket 166 attached to the side face of bar 1 by means of screw 167, and a thin flexible plate spring 168 clamped at one end to said bracket by means of screw 169 and attached at the other end to a coupling 170 by means ofwhich connection is made to the horizontal band 164.

The tension of the coil spring 153 on the spreader bar 152 keeps the bands 150, 1418, 162, 160, and 164.- taut, and it is plain that a horizontal oscillating motion of the frame A will impart a vertical oscillating motion to the vane V. The faces 158 and 159 of sector 155, and also the face of segment 133, all being segments of true cylinders, on which the several bands wrap themselves, it is evident that the amplitude of the motion of vane V will be proportional to that of the frame A.

Likewise, the band 148, being connected to'the true cylindrical face of segment 133 and bcmg wrapped onthe cylindrical surface of drum 136, the amplitude of the point 172 will i thereon the measure of the amplitude of the frame A.

The meter unit H is adjusted on the post 141st sueh arheight that when themne V isin a oe'ntrzilposition ,With respeotto thegpjole -pieces117,'the pointer 172 i p I the [dial 174. Also, the horizontal banda 164 Will stand at" on I is made e properllength so that when the pointer isiinthis positionlonthe dial, the bar s 1 Will rest injits neutral position midway-between the steps 67.- Adjustinent'for this neu- .tral position esefieoted byturning the thumb knobeel- The tension ofi theteke-up spring, or 153; onthe"'bar lithroughi the'mediuin of the by the torsion eonnected in a directleurrentf circuit, the source of supply be ngpreferably astorege battery; A-circuit is shown diagramn1atically' in Fig lrin' which the storage battery is designated. at The adjustment for flux 1 density ofthe magnetic field maybe eifected netic circuit; (by means V "strength' of the energizing 'current.= ter inethod being-the more s mple is here disi'closedf either by, varying'lthe reluctance of the mag- 1 of a ariable air gap oriotherWell'knoWn means)- or by arying the T he lat- Referrlng rheostetis indicated zit B, Whichisforgithe purpose of ad usting; i v

' directionv away from. the. disc niovement tothe strength 'ofthe current in the magnet coils, and an ainrneter is indicatedat I, which is providedso that, by proper adjustment of the 'rhe'ostztt R, the strength of the current, -I and hence the Insignia-tic v flux density in'ey be;

kept uniform Aswitch S isfprovided for closing and 'o'peningithe icireuit;

\ correctionsinay For the purpose of deterniining the redial direction-{er phase, of the resultant centrifugel force; or unbalance,

- locations; the ebov'ef'referred'to mechanism "designated by theletter'l) in Figures 1; 2, 3, i v V andb 'is proVided-f Referrhigfto'the detail" 7 vie'wsofthis ,unit,':FigsL2-O-to 24 inclusive; hnb portion 17'? is mounted onthei'end of shaft 25,- endsecu'red thereto by means ofe taper pin." Secu-red in'the-hub 7 portion 177 an'dextending therefroniin: a re:

dialfldire'ction ise stud-178.1 A weighti 1791s, slidably fitted on this stud, being liinited in Y Thei weight; '179 'isf, provlded,.onF'one side 7 W'ithjtWo transversely cut V 71118 811901 screws 185 itsslidingmoveijnen't irran outward direction byja head 180 endinaninward d rection by a fietgsurface 17 ion the-hub porti'on. r

f 81 and 182f spaced e'definite, distenceepert. gin'g these notches isfwlev er183', which upper end of thisrod. by means of; the knob accordingly.

l I 1 portion of I lever 183 I in the rotor. so that be applied thereon nproper' shaped notches supportsen'dfengagingfleonieel depressions inf the endsfin the said bar.

v 'llhel otherjen'dof le ver'il83 is bent at right angles asshown and i has its edgeV shaped to conform to the} "notohcs 181" and182'. "The middle? portion of the leveris enlarged a'nd provided ith an) "opening large enoughto clearthe hub portion 7' I '17 7 Which-projects through it. The V shaped maybe seen '11101'6 plainly in fFig; 22," this spring is secured to-eflu'g 189 int grmv t the disol'Zt} end its free endiests With pres-l sureagainstone side of einoteh a stud'IQO which is secured inthe lever 183es indicated;

portion 35 registers with the index mark on Thedisc unit-D is inounted onsh'eft25 in sncherelation to the gear heel" 35; thet,

when theab'ove referred to mark on its hub" clip 202, the rsicli al direction' ,of'the stud-17 8 is vertical.

.A secondhub portion froin the 1 front side of disc 176, the same being turned i 1 true-to fit thebore of a sleeve'192; Thissleeve is longitudinelly slottedjas s'hownlend pro- 1 "videdWith-lugs toreceive adjusting "screws 193 byiwhich it may be adjusted to ra close, yet i freely sliding fit'on the hub portion 191: A pin 194', secured in thewall of sleeve 192 operates in an 'el0ng2ited-fopening in hub 191, serving to prevent "turningeof the sleeye on san1e,'and to limit itssliding movement inthe Weird theidiso being limited the shoulder ylthereoni is i p r i Two studs .196 are secured indiametrically opposite positions" in lugs :19? on sleeve 192.

These studs extend through Isuiteble openl' thehand, i

o The. 11111: pertion of jidiscfl'l' is prcv-iiid with miseries of holes 199-; preferablyi 36 in nnmbensfinoed-IO 3 epa-rtiand disposed inn "circle, oneof-the holes 519:9" lyingin thegsenielf axial plane fasth'e stud-178?, Therholesfa re j ell lalike in diameter end ere taper-ed to fit f :thei shank 20 0 of a plug JFshowninTF-ig;24c,c 'so'thet it maybe pressed securely in, and by; twisting,ieasily removed fromany one of j *theholes'; 'In practice-several of these plugs f with head portions"ofdifferent Weights 'are 7,

provided for a purpose towbe leter'd'escribed,

On the peripherelfaceiof diso' l ifigendinre- (113111116 with the' hole's 199'arefsteinpednunn bars 0 to 180, indicating degrees, the number 0 being in line ,With the 1101511997. The

pose of the holes and; the plug; shown in Fig.

24 will beige; explained,"

can

The normal position of the weight 179 is that indicated in the figures; the V shaped end of lever 183 resting in the notch. 181. lVhilein this position the disc is placed in rotative balance, the same being effected by cutting away materialfrom lugs 201 which are provided for that purpose. The balancing operation is preferably performed while the'mechanism is mounted in place on the shafti25.

When the machine is operating and this unit'D is rotating, the weight 179 will, due to centrifugal force, tend to move outward on the stud. 178. If, while the rotation continues, the head 1980f sleeve 192 is pressed bythe hand of the operator, the lever 183 will. be pushed back by studs 196, and the weight-. 179 will move to its outward limit against" head 180 with notch 182 opposite the V shaped end'oflever 183. lVhen the pressure of the operators hand is released from the head 198 the lever 183 will, under the pressure of spring 188, move back to place with'the V shaped end in the notch 182 and hold. the weight in its new position. The disc is'thus thrown outof balance by a known amount dependingon the mass of weight 17 9'and the distance between the two notches 18l and 182 in same.

The preceding description covers the mechanism of a preferred form of machine embodying the invention. I will now proceed to describe the operation of same.

In the complete operation of balancing a rotative body, or rotor, the procedure is to make measurements (by means of the balano ing machine) which will indicate the magni tude of two corrections to-be appliedin two transverse planes, known as correction planes, located'a substantial distance apartalong the axis of rotation. The rotor isthen removed from the machine and the corrections determined -in the measuring operation are applied,

one in each plane, which will place the body in a state of running balance.

The unit for centrifugal force commonly employed iIrunbalance measurements the ounceinch, which-may bedefined as a centrif ugallforce'equal tothat produced by a'weight of one ounce revolving at a distance of 1 inch from the axis of rotation.

In machines ,of. the (type herein described, whatwe actuallynieasure is not the centrifugal force, but. rather, the movement of. the effective centrifugalforce about the pivotal axis .oni which the frame of the machine oscillates. Ill-,arrivingat the malgnitude of the correction ..to:a.pply,.the measured moment is dividedby thendistance of-thecorrec-i tion plane from the pivota'liaxis. The unit for the moment of force about the pivotal. axis is the ounce inch inch, which may be defined asthe moment ofa centrifugal-force of one ounce'inch, acting on the axis of rogenerated will be 1 ounce inch.

tation at. a distance of one inch from the pivotal axis.

In quantity production, where measuring One of the quantity of rotors to be balanced 1s first placed in perfect 1 running balance,

which may be accomplished in the machine by the slow, but well known and reliable method of applying trial weights successively in different positions in the correction planes until the result of perfect balance is obtained as evidenced by a zero reading of the ampli-. tude meter wlnle the rotation is at resonance speed. This perfectly balanced rotor is known asthe master rotor.

lVith the bolt 60 in raised position as shown in Fig. 4 this master rotor is mounted on the frame A as shown in 2. The bolt 60 is then lowered by means of handle (35 to the position shown in Fig. 5, thus releasing the frame and allowing it to swing freely between the limits of stops 67. An adjust. ment of the frame to neutral position, as indicated by the meter pointer 172 resting at 0, is then made by means of the thumb knob 54. The switch Sis then closed, thus energizing the magnet M, and the motor 21 is started. The rotor being in perfect balance, no oscillation will occur as will be evidenced by the pointer 172 ren iaining in its position of rest. The weight 179 on the disc unit is then released by pressing the hand against the head 198, allowing the weight to shift to its outer position, thus throwing the disc out of balance a known amount. The effect of this unbalance on the frame A will causeit to oscillate. The speed of rotation is then varied one way or the other by ll'lillllliillltltlllg the hand wheel 31 until resonancespeed is obtained, which is evidenced by the amplitude meter showing a maximum reading. The centrifugal force generated by the revolving weight 179, being a known quantity in the plane w-w, its moment about the pivotal axis P-P is also a known quantity. This quantity divided by the maximum reading noted, gives the moment per division on'the scale, which result is the calibration constant.

For example; assumng the weight 179to weigh 2 ounces, and the distance between the notches thereon inch, the centrifugal force suming the distance of plane wug from the pivot plane P'P to be 20 inches,.the moment of the centrifugal force will be 20 ounce inch Then as llU 7 v a 1nagnetYM ,rernaining energized, the motor slstarted; and the,inaxirnun vreadinglofthe.

I is

;nitude.ofthe correctlon in ounce inches to be, applied on the rotor in ;that plane. "Thus; continuing; the above example, ifthe maxi;

- f In a magnetic. damplng fdevice such as here-:

fwhere the iconstantl'ivill" be, unity; V give the advantage that", the; meter readings taken willfreprfesent directly the moment of iieously,

' therefroinl dam ingiforceiundei' I a ainplitudeidue to even'a slight unbalancewill beverygreat;;The amplitudefis then grad V u a'llfdecreased by increasing the dampingtorice untila. reading of'say 'lGi vd-iyisions' on thescale is rea' chedQ-Then by neierence-tio a nreviouslyj caleulated Chart, the unbalance I correspondingto the reading-- of anirneterl' I;

In the regular-i meter is obtained in the manner above deslcribedsiThe oscillation nowbeing due to the feentri'fu force generated; in-the rotor; the maximum reading of the inlet-er when lllLlltlplied by therca'l-ibration' constant; will give I the 'momene of this forceabout' the pivotal axis.= This; moment must be divided by the distance of thecor'rection plane'GC in the roto", fromthe axis F P to obtain the maginum reading WfiSiG divisions, the: moment of the centrifugal torcewouldl be 12 ounce, inch inches Then it the distance of the correction plane; from the pivotal axis] is 16 inches. the

tote-applied would be 12%;: 16911] correction .7 ouncelinches.

' 1 sityl of the magnetic field, so, evidently; the maximum-*- amplitude of oscillation flnay be? variedby 7 I hlnagnet M; I-As 'avineans for varying; the 'cur-- rent" is provided in the rheostat R,- it'ifs con-p venient, in v the operation of calibrating, to adjust the damping'forcethereb'y' toa'point V a This will varying the current strength in :the

1 1 3 "the centrifugal forcejanddo awayivith' the necessity of calculation; 7

It is obvious til tian certain arbitrary reading ofith'e niefiel isobf; V tainedl 'j'rThe reading :o iihe amnifeter-L nay thenbe'noted, and 'ithe unbalanceicelculated-f- Fo'r instance i at f the; start the rotat on may be; brought to resonance speed i while: the; adjustment islefor afverywslight:

which" condition a the i ches, li't mte lma i iunr g' he meter isilO' divisions on the scale, the moment perdivision; Will-be 20 divided by ['10, :or v2 ounce inchinches-Q Thus the calibration conlatent,WilllbeQ. i i i V V balancing operation,- the j calibration constant having been determined, 7 an unbalancedrotor is; mounted in the mav chinea'nd the weight179 is'pla'cedin its inner position with theldisic unit D in balancei The V be determined; Tl1-is.in'ethod however scribed method is preferred Y balance 7 is shifted by pressing. the on The centrifugal force then generated n the;

s .op'e i i n- After th eeniwtl at 111.1: hasbeen' measured n.j the manner above des'c-ri bed, and the HIa'XlDIUmI mBtGIL.

is cumbersome and therefore the/first I The phaseangle of thecentrifugal :iorce in the rotor is determlnediby a second ineasur disc will (exee'ptin rare instances) [be i r in a dil ierent direction thanthat aet ngjin the a rotor With thiseonditionexisting, a second the meter take'n? .vvill- .evidently represent theresultantfoif themeige forees one in the rotor andfthe other in "thel the eeil trifugalfl, 'forces'in bothrotor anddiso being known having been nieasure'db yj 5 bell'deterrninedl by inaxiinuni read ng-oI The nagnitudes of disc.

and. their resultant thelast operation, the phase' lof one-with re- ;-spect to the other may means of a force diagram as follows;

Reter representingby Weight 179. h Then iroin'wf as center,

ring to Fig. 29, a vertical-linen w is drawn; j

its length the nornent. of the a radius representing theinorne'nt of, the pen;

trifugalforce-generatedin therotorriis determined bythe first meter reading anarcfy is ems n; Then from 0 as center, with a radius V 2- representingthe resultant determined no the, ;in1 disclosed 1t vis x'vell known-that the damp; ing force generated dependsontheflux den i jdirection'of afline 0 n'drawnparalleltmw.m1 V

will be the direction offthe. centrifugalfforce i 1 se'eting the first are g atgtheipoint The generated in the disc, and theangle between};

angle of unbalance. J

phase angle I a v 1 i niorequickly than theconst-ruction of a alternatemethodZoi v imeas'uring 'the moment of centrifugal'j'fo i may .befelnnloyed; in which the speediot r .tationzis adjusted to T resonance; aillilfSllDllitfi theTheostatiR is adjusted'; until a angleqmayibe laid off and the-position pfjthe correction determined. i The procedurefiis with the index mark on clip 2 2, and treaty In praeticeit is desirable to. determine 7 the by reference to a table; injwhich I the angle. corresponding to successive values 1 of the; first and second rnete'r readings have 1 been calculated.- i Thusi the result is; obtained i no the lines 0 to and 0 nimay be-c'alled the phase I r Having: determined I the'nhase I necessary to establish-apointiin the-,corred; V tionplane on the rotorfromwhichthephase' asrfolloivsi therrotorfis' turned so that the" Inarlron -the hub face 35 ofgearf 35 V registers otdr-rn line with thisrnarkf After therotor '3 s removed fromsthe 'm'achin'e; the angle s' is V laid oft from the referenceniark andtheloca- It may be noted'that theirnethod above dev v .Qtion for the correctionisth-us-determined;

scribed does not indicate on which side of I the reference mark on the rotor to ley'ofi {the angle 4;. I For quantity productiondthe rotor is often; designed vvith .the: 

